The Simulation of a Surface Plasmon Resonance Metallic Grating for Maximizing THz Sensitivity in Refractive Index Sensor Application

Sathukarn, Asmar; Jia yi, Chia; Boonruang, Sakoolkan; Horprathum, Mati; Tantiwanichapan, Khwanchai; Prasertsuk, Kiattiwut; Thanapirom, Chayut; Kusolthossakul, Woraprach; Kasamsook, Kittipong

doi:https://doi.org/10.1155/2020/3138725

International Journal of Optics

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Abstract Introduction Characterization Conclusion Data Availability Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2020 | Article ID 3138725 | https://doi.org/10.1155/2020/3138725

The Simulation of a Surface Plasmon Resonance Metallic Grating for Maximizing THz Sensitivity in Refractive Index Sensor Application

Asmar Sathukarn,¹Chia Jia yi,¹Sakoolkan Boonruang,¹Mati Horprathum,¹Khwanchai Tantiwanichapan,¹Kiattiwut Prasertsuk,¹Chayut Thanapirom,¹Woraprach Kusolthossakul,¹and Kittipong Kasamsook¹

Academic Editor: Paramasivam Senthilkumaran

Received30 Sept 2019

Revised27 Nov 2019

Accepted28 Nov 2019

Published16 Jan 2020

Abstract

Nowadays, the simplicity of both designing and fabrication process of a terahertz (THz) resonator-based sensing technique leads to its ongoing development. The consumable THz resonator needs to be easily integrated into an existing terahertz time domain spectroscopy (THz TDS) measurement system. It should also be able to be fabricated in a mass scale with a low production cost. In this work, a metal-coated surface plasmon resonance- (SPR-) based sensor is simulated and designed as a low-cost refractive index sensor utilizing rigorous coupled wave analysis (RCWA). To demonstrate our methodology, we design a gold-coated grating with a polydimethylsiloxane (PDMS) as a substrate, in order to perform quantitative analysis of gasoline-toluene mixture composition, which has a refraction index variation of 0.1 at THz frequency. The grating period is tuned such that its surface plasmon resonance (SPR) frequency matches with the peak frequency of the THz TDS system. Moreover, other grating parameters, i.e., a filling factor and a grating depth, are optimized to increase the sensor sensitivity and sharpen the resonance dip. High sensitivity up to 500 GHz/RIU with a refractive index resolution up to 0.01 is numerically revealed. The H-field of the designed grating is then evaluated to indicate a strong SPR excitation. The well-developed designed grating introduces a promising, low-cost, and easily fabricated THz refractive index sensor.

1. Introduction

THz radiation is a part of an electromagnetic spectrum lying between microwaves and the far-infrared radiation (FIR). This region has frequencies ranging from 0.1 to 10 THz and wavelengths from 3 mm to 0.03 mm. THz radiation possesses properties inherited from both microwaves and IR. It is able to penetrate nonpolar materials, exhibits a high sensitivity towards moisture, and provides a specific response for each different material. At the same time, THz radiation is marked as safe to be used in a nondestructive evaluation due to its nonionizing nature. These unique properties of THz radiation can be utilized in many sensing applications [1] including those in the field of biology [2, 3], medical [4–7], and security [8, 9] and encouraging a comprehensive research and study.

The conventional THz sensing technique, which is usually performed by a THz TDS system, measures transmission or reflection spectral lines of molecular resonances while the molecules are illuminated with broadband THz radiation. This technique reaches its limit in detecting and analyzing a very small amount or a thin sample material. It requires a sufficient quantity or thickness to distinguish power or phase differences from the probing THz waves. The breakthrough of the detection limit could be achieved by the usage of the sensing devices [10], for example, a transmission line resonator [11], a metamaterial resonator [12], and a SPR sensor [13–16]. In general, all these devices could be described as a refractive index sensor detecting the minute change in a refractive index caused by a small amount of analytes placed in the active sensing region.

To enable the extensive uses of the THz sensing technique, the mass-producible, low-cost, and consumable THz resonators need to be easily integrated into an existing THz TDS measurement system. Among all the aforementioned sensing devices, the one-dimensional grating-based SPR is an attractive option due to its simplicity in both designing and fabrication process. In frequency ranges of visible light and IR, the PDMS has been introduced as a substrate material of a SPR grating to further simplify the fabrication process and reduce the fabrication cost [17–21]. For THz region, Nazarov et al. optimized SPR excitation on a metallic grating by varying grating parameters [22]. Subsequently, Spevak et al. and Lin et al. explored the role of material, especially semiconductors, for a THz SPR excitation [23, 24]. However, there is still a lack of research working on the low-cost THz SPR sensor.

In this work, a PDMS-based one-dimensional periodic rectangular THz SPR grating is proposed as a viable candidate of a THz refractive index sensor. Polydimethylsiloxane (PDMS) is low in cost, chemically stable, and biocompatible and easy for fabrication, via soft lithography or pattern transfer, supporting its use in many applications [25]. The THz SPR grating is numerically simulated based on RCWA. A purposed workflow for a grating structure design is created and demonstrated through an example of THz sensing application, i.e., the quantitative analysis of a petrochemical. This could be a guidance for designing the SPR grating in other refractive index range using the THz sensing technique.

2. Numerical Method

Surface plasmon resonance (SPR) is a coupling phenomenon of a transverse magnetic (TM) mode of an electromagnetic field of an incident wave and a collective oscillation of a free electron that is located at the boundary between the dielectric and metal [26]. These phenomena have been used in many applications, particularly, for sensing purposes [27–30]. In order to excite surface plasmons, the phase matching condition needs to be satisfied. In general case for SPR, the wave vector of the incident wave () needs to be matched with the wave vector of a surface wave () based on the conservation of the momentum which can be expressed aswhere is the permittivity of a metal and is the refractive index of a dielectric.

For the diffraction of light in the metallic grating, the wave vector of a diffracted light parallel to the grating surface is equal to the propagation constant of the surface plasmon. To be more specific, the diffraction order m^th is required to couple to the surface wave:where is the angle of an incidence beam and is the grating period. Therefore, substituting from (1) into (2) gives the matching condition of SPR, which can be expressed as

Generally, the effective excitation of the surface plasmon requires . This leads to the determination of diffraction orders from the frequency response, which is controlled by the grating period [31, 32]:

In order to optimize the excitation condition, the analytical study of SPR excitation model has been developed by using a RCWA. RCWA formulation is numerically stable for solving the Maxwell equations at a single layer binary or a planar grating, especially the numerical instability in the matching of electromagnetic field at the dielectric and metal interface [33]. The Drude model is also used to derive the dispersion relation of the SPR propagating on a one-dimensional rectangular metal coated grating. Figure 1 shows the grating structure with a grating period , a grating width W, a grating depth H, and a metal thickness t_m.

3. Grating Design and Characterization

In order to conceptualize the application of a SPR grating in THz sensing, the designing of an optimized grating for quantitative analysis of petrochemical and their mixture is showcased. This designed grating could be applied to other THz sensing application with the extended refractive index range. Because of the nonpolar nature of the petrochemical and organic solvent, THz spectroscopy has a great potential to be applied in analysis of liquid petrochemicals and their mixtures with an organic solvent. Researchers have studied molecular properties of petrochemical products in the THz range and demonstrated the qualitative and quantitative analyses of liquid petrochemicals by using a THz TDS system [34].

In this work, we numerically design a metal-coated PDMS SPR grating for improving a detection sensitivity of the THz TDS in analyzing a gasoline-toluene mixture, which has a refractive index lying between 1.4 and 1.5 in the frequency range of 0.2 to 2.0 THz [35, 36]. The proposed experiment setup is illustrated in Figure 2. An analyte is coated on the grating surface, and the resonance frequency shift of the THz spectrum is detectable resulting from the difference in the refraction index. The resonance frequency of the designed grating is aimed to be at 1 THz or lower because most of the photoconductive antenna- (PCA-) based THz TDS is limited by a bandwidth of approximately 5 THz, and the center frequency is less than 1 THz [37].

3.1. Design and Optimization Process

The grating structure considered here, as shown in Figure 1, is composed of a PDMS substrate coated by a gold (Au) film, which is a perfect electric conductor in THz range. The complex refractive indices of PDMS and Au film are assigned as n_s = 1.533 − j0.034 [38] and n_m = 447 − j532 [39], respectively. The metal thickness t_m is an important factor for improving a sensor performance depending on the coupling configuration and structure. For example, the Au thickness affects the sensitivity of a SPR fiber grating biosensor [40]. In this study, measuring in a reflection mode, t_m is set to be 100 nm, which is larger than the skin depth of Au (l_s,Au = 74 nm) in the frequency of interest [41]. We assume that, in the case of t_m > l_s,Au, there is no radiative loss of resonance arising from the diffraction on the grating. Theoretically, a small incident angle of TM excitation wave would maximize the electric field on the grating structure. The incident angle of the incoming wave is set to be 10°, which is the minimum angle required in an actual TDS reflection measurement setup.

The geometrical parameters of a grating structure include Λ, H, and FF, which is a ratio of W and Λ. Based on (3), Λ is the first parameter to be varied in the grating optimization as it is directly related to the resonance frequency of the SPR. FF and H of the initial structure are set at 0.5 and 0.5Λ, respectively. The refractive index of the dielectric, a gasoline analyte coated on the SPR grating, is taken as n_d = 1.4. In this simulation, Λ is varied from 150 μm to 250 μm, with a step of 10 μm to figure out the appropriate Λ of the grating with a resonance frequency of 1 THz.

The result shows that the suitable Λ is 190 μm. Figure 3 shows two reflectance dips existed in the range of 0.5 to 1.5 THz, located at 0.984 THz and 1.274 THz, respectively. According to (4) and (5), these peaks corresponded to the diffraction order m of 1 and −1, respectively. This can be indicated that the resonance or plasmonic peak can be coupled into the surface by such a designed structure. The inset of Figure 3 demonstrates the distribution of a magnetic field magnitude |H_y| along the unit cell of the grating at the resonance frequency of 0.984 THz. The structure of the 190 μm Λ grating needs to be further optimized by varying FF and H, which are directly related to the coupling efficiency, to minimize the reflectance of the resonance peak (reflectance R = 0.77 at 0.985 THz). While H is remained at 0.5Λ, the FF of a grating, which is proportional to W, is the second parameter to be varied. An appropriate W of the grating satisfies the coupling condition and enhances the confinement of the surface plasmon electric field on the grating surface.

In the optimization process, figure of merit (FOM), defined as the ratio between sensitivity (S) and the full width half max (FWHM) of a reflectance dip, is used to evaluate the performance of a grating structure [42]. The term of sensitivity S is known as the rate of change of a resonance frequency with respect to a refraction index of the analyte:

In this study, FF is varied from 0.5 to 0.9 with a step of 0.05. The optimum FF of the 190 μm Λ grating is found in the range of 0.7 to 0.9, which is corresponding to W of 133 to 171 μm, giving the reflectance of less than 0.1, as illustrated in Figure 4(a). The resonance reflection dip is shifted to a lower frequency as FF increases. The FOM plot, as shown in Figure 4(b), shows that the grating with FF of 0.8, which has R = 0.019 at = 0.851 THz, is superior among all the gratings.

(a)

(b)

The parameter, H, is varied from 75 to 115 μm with a step of 10 μm, to fine-tune the performance of the grating. In correspondence to the optimized W, an appropriate H is needed to achieve a critical coupling condition whereby a reflection from the grating is suppressed and maximum power is transferred to the surface plasmon polaritons [43, 44]. Based on the plots in Figure 5(a), H of 85 μm is the optimum depth for this SPR grating providing the highest FOM. S of this optimized grating structure is approximately 500 GHz/refraction index unit (RIU) in the refractive index range of 1.4 to 1.5 (maximum S = 559 GHz/RIU at n = 1.44). Figure 5(b) shows the sensitivity of the designed grating as a function of a refractive index while its inset shows the calculated resonance frequency in analyzing the gasoline-toluene mixture. As most of the commercial THz TDS system could achieve a spectral resolution of less than 5 GHz, the sensitivity of this SPR grating could detect the change in the refractive index of the analyte as low as 0.01.

(a)

(b)

Figure 5

(a) FOM as a function of refractive index with a variation of H in an Au-coated PDMS grating with Λ = 190 μm, FF = 0.8, and t_m = 100 nm at the incident angle of 10°. (b) Sensitivity plot of the interested refractive range, 1.4 to 1.5, of the optimized grating structure with Λ = 190 μm, FF = 0.8, H = 85 μm, and t_m = 100 nm at the incident angle of 10°. The inset shows the resonance frequency f₀ of this grating for different compositions of gasoline-toluene mixture.

The reflectance of the optimized grating geometry with Λ of 190 μm, FF of 0.8, and H of 85 μm shows a SPR dip in the frequency range of 0.5 to 1.5 THz, with the reflectance of 3.59 × 10⁻⁴ located at the resonance frequency of 0.869 THz corresponding to the diffraction order m = 1, as depicted in Figure 6(a). It can be noted that the designed structure satisfies the phase matching condition. Numerically, the H_y field distribution on the grating surface at the resonance frequency reveals that the resonance is intense and localized at the dielectric and Au interface, as presented Figure 6(b). This indicates that the decay length of the SPR wave at the dielectric and Au interface is high enough to form SPR mode. In comparison, the |H_y| intensity of the optimized structure is 4 times higher that of the initial structure, as shown in Figure 3. Table 1 shows the optimized grating parameters found in this study.

(a)

(b)

4. Conclusion

In this study, we have proposed a parameter design methodology for a one-dimensional periodic rectangular metallic grating design to be used in a THz refractive index sensor application. The sensor detects the refractive index of the coating analyte by using a THz TDS system to measure the shift of the grating surface plasmon resonance frequency. Our design methodology begins by varying the grating period in order to tune its resonance frequency in presence of the analyte to match the peak power frequency of the THz TDS system. Then, other relevant grating parameters of its FF and H are varied to maximize the detection FOM.

The design process is demonstrated in which Au-coated PDMS-based grating is numerically simulated with a purpose of quantitatively analyzing gasoline-toluene mixture composition. The optimized SPR grating presents a sensitivity of 500 GHz/RIU resulting in a refractive index detection resolution of 0.01 RIU, which is superior to a direct measurement method. A further experimental verification of our grating design is still needed as a future work. The proposed structure could be fabricated via a standard PDMS casting and curing method following by a thin Au film layer deposition with a conventional metal deposition technique. Furthermore, the SPR grating could be utilized in other refractive index range by applying such a THz sensing technique.

Data Availability

The data used to support the findings of this study are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

This work was financially supported by the National Electronics and Computer Technology Center (NECTEC), NSTDA, Thailand, under a funded project (P1750977).

References

M. J. Fitch and R. Osiander, “Terahertz waves for communications and sensing,” Johns Hopkins APL Technical Digest (Applied Physics Laboratory), vol. 25, no. 4, pp. 348–355, 2004.
View at: Google Scholar
C. Situ, M. H. Mooney, C. T. Elliott, and J. Buijs, “Advances in surface plasmon resonance biosensor technology towards high-throughput, food-safety analysis,” TrAC Trends in Analytical Chemistry, vol. 29, no. 11, pp. 1305–1315, 2010.
View at: Publisher Site | Google Scholar
J. Zhou, Q. Qi, C. Wang et al., “Surface plasmon resonance (SPR) biosensors for food allergen detection in food matrices,” Biosensors and Bioelectronics, vol. 142, Article ID 111449, 2019.
View at: Publisher Site | Google Scholar
A. Dhawan, M. Canva, and T. Vo-Dinh, “Narrow groove plasmonic nano-gratings for surface plasmon resonance sensing,” Optics Express, vol. 19, no. 2, pp. 787–813, 2011.
View at: Publisher Site | Google Scholar
B. Ng, S. M. Hanham, J. Wu et al., “Broadband terahertz sensing on spoof plasmon surfaces,” ACS Photonics, vol. 1, no. 10, pp. 1059–1067, 2014.
View at: Publisher Site | Google Scholar
A. Alipour, A. Farmani, and A. Mir, “High sensitivity and tunable nanoscale sensor based on plasmon-induced transparency in plasmonic metasurface,” IEEE Sensors Journal, vol. 18, no. 17, pp. 7047–7054, 2018.
View at: Publisher Site | Google Scholar
V. V. Bulgakova, V. V. Gerasimov, B. G. Goldenberg, A. G. Lemzyakov, and A. M. Malkin, “Study of terahertz spoof surface plasmons on subwavelength gratings with dielectric substance in grooves,” Procedia Engineering, vol. 201, pp. 14–23, 2017.
View at: Publisher Site | Google Scholar
J. F. Federici, B. Schulkin, F. Huang et al., “THz imaging and sensing for security applications-explosives, weapons and drugs,” Semiconductor Science and Technology, vol. 20, no. 7, pp. S266–S280, 2005.
View at: Publisher Site | Google Scholar
A. G. Davies, A. D. Burnett, W. Fan, E. H. Linfield, and J. E. Cunningham, “Terahertz spectroscopy of explosives and drugs,” Materials Today, vol. 11, no. 3, pp. 18–26, 2008.
View at: Publisher Site | Google Scholar
J. F. O’Hara, W. Withayachumnankul, and I. Al-Naib, “A review on thin-film sensing with terahertz waves,” Journal of Infrared, Millimeter, and Terahertz Waves, vol. 33, no. 3, pp. 245–291, 2012.
View at: Publisher Site | Google Scholar
T. Akalin, A. Treizebre, and B. Bocquet, “Single-wire transmission lines at terahertz frequencies,” IEEE Transactions on Microwave Theory and Techniques, vol. 54, no. 6, pp. 2762–2767, 2006.
View at: Publisher Site | Google Scholar
M. Islam, S. J. M. Rao, G. Kumar, B. P. Pal, and D. Roy Chowdhury, “Role of resonance modes on terahertz metamaterials based thin film sensors,” Scientific Reports, vol. 7, no. 1, p. 7355, 2017.
View at: Publisher Site | Google Scholar
K. A. Willets and R. P. Van Duyne, “Localized surface plasmon resonance spectroscopy and sensing,” Annual Review of Physical Chemistry, vol. 58, no. 1, pp. 267–297, 2007.
View at: Publisher Site | Google Scholar
J. Homola, S. S. Yee, and G. Gauglitz, “Surface plasmon resonance sensors: review,” Sensors and Actuators B: Chemical, vol. 54, no. 1-2, pp. 3–15, 1999.
View at: Publisher Site | Google Scholar
D. Shankaran, K. Gobi, and N. Miura, “Recent advancements in surface plasmon resonance immunosensors for detection of small molecules of biomedical, food and environmental interest,” Sensors and Actuators B: Chemical, vol. 121, no. 1, pp. 158–177, 2007.
View at: Publisher Site | Google Scholar
T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through sub-wavelength hole arrays,” Nature, vol. 391, no. 6668, pp. 667–669, 1998.
View at: Publisher Site | Google Scholar
W.-H. Yeh, J. Kleingartner, and A. C. Hillier, “Wavelength tunable surface plasmon resonance-enhanced optical transmission through a chirped diffraction grating,” Analytical Chemistry, vol. 82, no. 12, pp. 4988–4993, 2010.
View at: Publisher Site | Google Scholar
A. Ryabchun, M. Wegener, Y. Gritsai, and O. Sakhno, “Novel effective approach for the fabrication of PDMS‐based elastic volume gratings,” Advanced Optical Materials, vol. 4, no. 1, pp. 169–176, 2016.
View at: Publisher Site | Google Scholar
P. Gutruf, E. Zeller, S. Walia, S. Sriram, and M. Bhaskaran, “Mechanically tunable high refractive-index contrast TiO2-PDMS gratings,” Advanced Optical Materials, vol. 3, no. 11, pp. 1565–1569, 2015.
View at: Publisher Site | Google Scholar
B. Sheng, L. Luo, Y. Huang, G. Chen, H. Zhang, and S. Zhuang, “Tailorable elastomeric grating with tunable groove density gradient,” IEEE Photonics Journal, vol. 9, no. 5, pp. 1–6, 2017.
View at: Publisher Site | Google Scholar
W. Liu, Y. Shen, G. Xiao, X. She, J. Wang, and C. Jin, “Mechanically tunable sub-10 nm metal gap by stretching PDMS substrate,” Nanotechnology, vol. 28, no. 7, Article ID 075301, 2017.
View at: Publisher Site | Google Scholar
M. Nazarov, F. Garet, D. Armand, A. Shkurinov, and J.-L. Coutaz, “Surface plasmon THz waves on gratings,” Comptes Rendus Physique, vol. 9, no. 2, pp. 232–247, 2008.
View at: Publisher Site | Google Scholar
I. S. Spevak, A. A. Kuzmenko, M. Tymchenko et al., “Surface plasmon-polariton resonance at diffraction of THz radiation on semiconductor gratings,” Low Temperature Physics, vol. 42, no. 8, pp. 698–702, 2016.
View at: Publisher Site | Google Scholar
S. Lin, K. Bhattarai, J. Zhou, and D. Talbayev, “Giant THz surface plasmon polariton induced by high-index dielectric metasurface,” Scientific Reports, vol. 7, no. 1, p. 9876, 2017.
View at: Publisher Site | Google Scholar
S. Alfihed, M. H. Bergen, J. F. Holzman, and I. G. Foulds, “A detailed investigation on the terahertz absorption characteristics of polydimethylsiloxane (PDMS),” Polymer, vol. 153, pp. 325–330, 2018.
View at: Publisher Site | Google Scholar
W. L. Barnes, A. Dereux, and T. W. Ebbesen, “Surface plasmon subwavelength optics,” Nature, vol. 424, no. 6950, pp. 824–830, 2003.
View at: Publisher Site | Google Scholar
S. Nair, C. Escobedo, and R. G. Sabat, “Crossed surface relief gratings as nanoplasmonic biosensors,” ACS Sensors, vol. 2, no. 3, pp. 379–385, 2017.
View at: Publisher Site | Google Scholar
J.-Y. Jing, Q. Wang, W.-M. Zhao, and B.-T. Wang, “Long-range surface plasmon resonance and its sensing applications: a review,” Optics and Lasers in Engineering, vol. 112, pp. 103–118, 2019.
View at: Publisher Site | Google Scholar
Y. Si, J. Lao, X. Zhang et al., “Electrochemical plasmonic fiber-optic sensors for ultra-sensitive heavy metal detection,” Journal of Lightwave Technology, vol. 37, no. 14, pp. 3495–3502, 2019.
View at: Publisher Site | Google Scholar
S. Mariani and M. Minunni, “Surface plasmon resonance applications in clinical analysis,” Analytical and Bioanalytical Chemistry, vol. 406, no. 9-10, pp. 2303–2323, 2014.
View at: Publisher Site | Google Scholar
K. Lin, Y. Lu, J. Chen, R. Zheng, P. Wang, and H. Ming, “Surface plasmon resonance hydrogen sensor based on metallic grating with high sensitivity,” Optics Express, vol. 16, no. 23, pp. 18599–18604, 2008.
View at: Publisher Site | Google Scholar
C. Hu and D. Liu, “High-performance grating coupled surface plasmon resonance sensor based on Al-Au Bimetallic layer,” Modern Applied Science, vol. 4, no. 6, p. 8, 2010.
View at: Publisher Site | Google Scholar
M. G. Moharam, T. K. Gaylord, D. A. Pommet, and E. B. Grann, “Stable implementation of the rigorous coupled-wave analysis for surface-relief gratings: enhanced transmittance matrix approach,” Journal of the Optical Society of America A, vol. 12, no. 5, pp. 1077–1086, 1995.
View at: Publisher Site | Google Scholar
M. Yin, S. Tang, and M. Tong, “The application of terahertz spectroscopy to liquid petrochemicals detection: a review,” Applied Spectroscopy Reviews, vol. 51, no. 5, pp. 379–396, 2016.
View at: Publisher Site | Google Scholar
Y. S. Jin, G. J. Kim, C.-H. Shon, S. G. Jeon, and J. I. Kim, “Analysis of petroleum products and their mixtures by using terahertz time domain spectroscopy,” Journal of the Korean Physical Society, vol. 53, no. 4, pp. 879–1885, 2008.
View at: Publisher Site | Google Scholar
G.-J. Kim, S.-G. Jeon, J.-I. Kim, and Y.-S. Jin, “Terahertz time domain spectroscopy of petroleum products and organic solvents,” in Proceedings of the 2008 33rd International Conference on Infrared, Millimeter and Terahertz Waves, Pasadena, CA, USA, September 2008.
View at: Publisher Site | Google Scholar
Y. Zhang, X. Zhang, S. Li et al., “A broadband THz-TDS system based on DSTMS emitter and LTG InGaAs/InAlAs photoconductive antenna detector,” Scientific Reports, vol. 6, no. 1, p. 26949, 2016.
View at: Publisher Site | Google Scholar
M. Querry, Optical Constants of Minerals and Other Materials from the Millimeter to the Ultraviolet, Chemical Research Development and Engineering Center Aberdeen Proving Groundmd, USA, 1987.
M. A. Ordal, R. J. Bell, R. W. Alexander, L. L. Long, and M. R. Querry, “Optical properties of Au, Ni, and Pb at submillimeter wavelengths,” Applied Optics, vol. 26, no. 4, pp. 744–752, 1987.
View at: Publisher Site | Google Scholar
C. Caucheteur, M. Loyez, Á. González-Vila, and R. Wattiez, “Evaluation of gold layer configuration for plasmonic fiber grating biosensors,” Optics Express, vol. 26, no. 18, pp. 24154–24163, 2018.
View at: Publisher Site | Google Scholar
S. Nagai, T. Hayashi, and A. Sanada, “Measurements of anomalous skin effect in 1 THz band,” in Procedings of the 2013 IEEE MTT-S International Microwave Symposium Digest (MTT), pp. 1–3, Seattle, WA, USA, June 2013.
View at: Publisher Site | Google Scholar
X. Qiu, X. Chen, F. Liu, B.-O. Guan, and T. Guo, “Plasmonic fiber-optic refractometers based on a high Q-factor Amplitude interrogation,” IEEE Sensors Journal, vol. 16, no. 15, pp. 5974–5978, 2016.
View at: Publisher Site | Google Scholar
H. Hori, K. Tawa, K. Kintaka, J. Nishii, and Y. Tatsu, “Influence of groove depth and surface profile on fluorescence enhancement by grating-coupled surface plasmon resonance,” Optical Review, vol. 16, no. 2, pp. 216–221, 2009.
View at: Publisher Site | Google Scholar
S. T. Koev, A. Agrawal, H. J. Lezec, and V. A. Aksyuk, “An efficient large-area grating coupler for surface plasmon polaritons,” Plasmonics, vol. 7, no. 2, pp. 269–277, 2012.
View at: Publisher Site | Google Scholar

Copyright

Copyright © 2020 Asmar Sathukarn et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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